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8.6 Toy Monte Carlo study 117<br />

80<br />

[pb]<br />

σ excl<br />

tot<br />

60<br />

40<br />

20<br />

B C D E F<br />

0<br />

Figure 8.9: The exclusive photon plus jet total cross sections obtained with five different<br />

unfoldings. The inner error bars represent the statistical error, outer error bars statistical<br />

and systematic added in quadrature. The shaded area and horizontal lines indicate error<br />

ranges for the unfolding B.<br />

is subject to the unfolding procedure and the results are compared to the known MC<br />

distribution. Three sets of toy MC samples were produced for the purpose of this analysis<br />

by reweighting the original MC set I:<br />

• The set of seven reweighting functions fE x T<br />

designed to reweight the MC E γ T distribution<br />

in such a way that the reweight value for events with E γ T<br />

= 6 GeV is equal<br />

to one, while events with E γ T<br />

= 15 GeV are weighted up by x percentage:<br />

fE x T<br />

= x × E γ T<br />

/900 GeV − x/150 − 1, (8.43)<br />

with the chosen x values are taken from the set 5, <strong>10</strong>, 20, 50, <strong>10</strong>0, 150, 250.<br />

• The set of seven reweighting functions f x η designed to reweight the MC ηγ distribution<br />

in such a way that the reweight value for events with η γ = −1 is equal to one,<br />

while events with η γ = 2.4 are weighted up by x percentage:<br />

f x η = x × η γ /340 + x/340 + 1, (8.44)<br />

with the chosen x values are taken from the set 5, <strong>10</strong>, 20, 50, <strong>10</strong>0, 150, 250.<br />

• The double dimensional E γ T − ηγ reweighting function f toy<br />

E T ,η<br />

produced to test the<br />

unfolding in the extreme case. The function implements reweighting in η γ corresponding<br />

to f 450<br />

η<br />

from f 350<br />

E T<br />

up to even f 1<strong>10</strong>0<br />

convoluted with non linear reweighting in E γ T<br />

E T<br />

:<br />

of the scale ranging<br />

f toy<br />

E T ,η = (Eγ T /GeV )2 /40 + η γ /2 (8.45)

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